Engineering luminopsins with improved coupling efficiencies

Abstract. Significance Luminopsins (LMOs) are bioluminescent-optogenetic tools with a luciferase fused to an opsin that allow bimodal control of neurons by providing both optogenetic and chemogenetic access. Determining which design features contribute to the efficacy of LMOs will be beneficial for further improving LMOs for use in research. Aim We investigated the relative impact of luciferase brightness, opsin sensitivity, pairing of emission and absorption wavelength, and arrangement of moieties on the function of LMOs. Approach We quantified efficacy of LMOs through whole cell patch clamp recordings in HEK293 cells by determining coupling efficiency, the percentage of maximum LED induced photocurrent achieved with bioluminescent activation of an opsin. We confirmed key results by multielectrode array recordings in primary neurons. Results Luciferase brightness and opsin sensitivity had the most impact on the efficacy of LMOs, and N-terminal fusions of luciferases to opsins performed better than C-terminal and multi-terminal fusions. Precise paring of luciferase emission and opsin absorption spectra appeared to be less critical. Conclusions Whole cell patch clamp recordings allowed us to quantify the impact of different characteristics of LMOs on their function. Our results suggest that coupling brighter bioluminescent sources to more sensitive opsins will improve LMO function. As bioluminescent activation of opsins is most likely based on Förster resonance energy transfer, the most effective strategy for improving LMOs further will be molecular evolution of luciferase-fluorescent protein-opsin fusions.


Introduction
Manipulation of neuronal activity in behaving experimental animals is crucial for elucidating neuronal networks underlying brain function.Both optogenetic 1 and chemogenetic 2 approaches continue to be highly valuable for identifying the contributions of genetically defined neuron populations to circuit and behavioral outputs.Both methods offer distinct advantages, with optogenetic control of the activity of subsets of neurons at precise temporal scales and slower chemogenetic control of the activity of entire populations of neurons across the brain.Previous work has developed a toolset that integrates opto-and chemogenetic approaches by fusing a light-emitting luciferase to an optogenetic light-responsive element, resulting in a luminescent opsin, or luminopsin (LMO) [3][4][5] [Fig.1(a)].Bioluminescence produced by oxidation of a diffusible luciferin substrate by the luciferase enzyme activates a tethered, nearby opsin.Depending on the biophysical properties of the opsin, the light generated by the luciferase can either excite or inhibit target neurons expressing the LMO.Such integration of opto-and chemogenetic approaches allows manipulation of neural activity over a range of spatial and temporal scales of the same neurons in the same experimental animal.For example, the contribution to behavioral components of the activation of an entire population of neurons can be compared to those of a subset of the same neurons, activating the opsin chemogenetically through bioluminescence or optogenetically through light fibers. 6or the first excitatory LMO1, wild type luciferase (GLuc) 7 was combined with channelrhodopsin 2 (ChR2). 8While application of luciferin induced small inward currents in HEK293 cells, bioluminescence was not able to generate action potentials in neurons. 3Efficiently changing membrane potentials in neurons required the use of a brighter light emitter such as the GLuc variant "slow burn" (sbGLuc) 9 in combination with optogenetic channels with higher light sensitivity, such as Volvox channelrhodopsin 1 (VChR1). 10,113][14][15][16][17][18][19] We and others have since continued to combine more potent light emitters with more light sensitive opsins to generate LMOs with still higher efficacies.These efforts include use of novel luciferase mutants, such as GLucM23, 20 molecularly evolved luciferase-fluorescent protein fusions, such as NCS2 (eKL9h-mNeonGreen), 21 and opsins with higher light sensitivities, such as step function opsins. 22hese further improvements in LMO efficacy enable more effective neuron activation with less luciferin or via easier application routes (for example, intraperitoneal instead of intravenous).Taking advantage of new developments and discoveries in optogenetic tools, such as the machine learning-guided engineering of the designer channelrhodopsin ChRger 23 and the discovery of the marine opsin ChRmine from Tiarina fusus 24 together with recent progress in further evolving luciferases (SSLuc 25 ), we have continued to generate new versions of LMOs (Table 1).Design principles in addition to brightness of luciferases and sensitivity of opsins were the arrangement of moieties and the wavelength compatibility of emitter and sensor [Figs.1(b) and 1(c)].The moieties of LMOs can be arranged in one of three ways, with the luciferase on the N-terminus, C-terminus, or both the N-and C-termini of the opsin [Fig.1(c)].In all our previous designs, the luciferase was tethered to the N-terminus of the opsin.However, for the inhibitory iLMO2, 4 the RLuc-based luciferase-fluorescent fusion protein Nanolantern 26 was tethered to the C-terminus of the opsin Natronomonas halorhodopsin (NpHR). 27Each luciferase and opsin partnered for an LMO has a unique peak emission and absorption spectrum, respectively [Fig.1(b)].We hypothesized that closely matching these spectra will improve the function of LMOs.
To compare the efficacy of different LMOs in changing a cell's membrane potential, we assessed eight excitatory LMOs through whole cell patch clamp recordings in HEK293 cells.By measuring the amplitude of inward current elicited with a metal halide light source versus the one elicited by bioluminescence, we were able to calculate for each LMO the coupling efficiency, the percentage of optogenetic activation of an opsin that can be achieved with bioluminescent stimulation. 3We used this quantification of the efficacy of a light emitter-light sensor pairing to identify which design characteristics of LMOs are most impactful.

Plasmids
Plasmids were cloned with conventional molecular biology techniques.Some constructs were cloned into both pcDNA and pAAV vectors for testing in HEK293 cells and primary neurons, respectively.Constructs are listed in Table 2.

Virus
AAVs carrying LMOs were produced by transfecting subconfluent HEK293FT cells per 10-cm culture dish with 24 μg of the helper plasmid pAd delta F6, 20 μg of the serotype plasmid AAV2/ 9, and 12 μg of the LMO plasmid using lipofectamine 2000.After 72 h, the supernatant was harvested from culture plates and filtered at 0.45 μm.Virus was purified from cells and supernatant according to previously described methodology, 28 but without the partitioning step in the aqueous two-phase system.Virus was dialyzed against PBS (w/o Ca, Mg) overnight at 4°C, using FLOAT-A-LYZER G2, MWCO 50 kDa, followed by concentration in Amicon Ultra-0.5 379 mL centrifugal filters.Viral titers were determined by quantitative PCR for the woodchuck hepatitis
Cells were plated on one-well multielectrode array (MEA) plates (60MEA200/30iR-Ti; Multichannel Systems) at a seeding density of 7 × 10 4 in a 10 μl drop. 29,30Once the cells had adhered to the surface, the wells were slowly flooded with NB-FCS and plates were returned to the incubator.Viral transduction of constructs occurred the next day (∼18 to 24 h) together with changing to culture medium without serum (NB-Plain: neurobasal medium, 2% B-27, 2 mM Glutamax, 0.1% gentamycin).Three days later media was changed to Neurobasal Plus Medium (Invitrogen), with 2% B-27 Plus supplement (Gibco, ThermoFisher), 2 mM Glutamax, and 0.1% gentamycin (NB+).Every 3 to 4 days a third of media was replaced with fresh NB+.Cells were maintained in a 5% CO 2 atmosphere at 37°C.

HEK Cell Electrophysiology
Whole cell voltage patch clamp was performed on HEK293 cells 24 to 72 h after transfection.A coverslip was transferred to a recording chamber (RC26-GLP, Warner Instruments) on the stage of an upright microscope (BX51WI, Olympus) and perfused with external buffer (1.5 mL∕ min)  w/BX2 cube) excitation.An electronic shutter (Lambda SC, Sutter Instruments) was used to control light delivery to cells and limit exposure to 1 s.Photocurrents were evoked with blue, green, or red light to match the peak bioluminescence emission of the luciferase tethered to the opsin.At maximum, light intensity from the light source irradiance was (in mW∕cm 2 ) 16.8, 36.5, and 39.9, respectively, as measured with a light meter (ThorLabs).

Multi Electrode Array Recordings
MEA2100-Lite-System (Multichannel Systems, Germany) was used for all MEA recordings with Multichannel Experimenter software at a sample rate of 10,000 Hz.Consistently spiking neurons were used for recordings between DIVs 14 and 25; only cultures showing spontaneous electrophysiological activity were used.All-trans retinal (R2500; Sigma-Aldrich, St. Louis, Missouri) was added to the culture medium to 1 μM final concentration before electrophysiological recordings.Prior to recording, all reagents were pre-warmed to 37°C.MEAs were transferred from the CO 2 incubator to the heated MEA2100 head stage maintained at 37°C, and the cultures were allowed to equilibrate for 5 to 10 min.The headstage was situated on a support stage with a PlexBright optical patch cable positioned from below to illuminate the center of the MEA dish.The patch cable was connected to a Plexon optogenetic LED fiber-coupled module (blue, 465 nm; green, 525 nm; lime, 550 nm) controlled by a PlexBright LD-1 single channel LED driver for light stimulation of cultures at different wavelengths.A micropipette was used to add luciferin or vehicle with the reagent drop gently touching the liquid surface, creating a timelocked artifact in the recordings.After recording, the media in the wells were replaced with fresh pre-equilibrated and pre-warmed NB-Plain media, and the cultures were used for another round of recording the next day.

HEK cell electrophysiology
Recordings were sampled at 10 kHz.Photocurrents were assessed in Clampfit (Molecular Devices) at steady state level during the last 100 ms of illumination to eliminate inconsistencies found before light-adaptation during peak current response.Luciferin-induced currents were measured in Clampfit where the amplitude plateaus during stimulation.Coupling efficiencies were determined by normalizing luciferin-induced current change to photocurrent change elicited by the lamp (i.e., luciferin-induced current/photocurrent).In non-expressing controls, LED and luciferin impact on current was determined.All traces were sampled at 10 kHz and filtered on Clampfit using a Gaussian lowpass filter with a 250 Hz to 3 dB cutoff before displaying in figures.

MEA recordings
All MEA analysis was done offline with Multichannel Analyzer software (Multichannel Systems) and NeuroExplorer (RRID: SCR_001818).Spikes were counted when the extracellular recorded signal exceeded nine standard deviations of the baseline noise.For assessing the effects of CTZ (10 μm final concentration), only electrodes displaying the expected change in spiking activity with blue light from the LED light source, i.e., opsin expressing neurons, were evaluated.Spikes were counted before luciferin or vehicle was added and immediately after addition.Spike frequency was also assessed for LED exposure.Pooled data was obtained from different electrodes (a) of the same culture, (b) from different cultures, and (c) over different DIVs.
To evaluate the significance of differences in firing rate across conditions and groups, we performed a permutation test.This non-parametric approach allowed us to compare neuronal firing rates between pre-and post-treatment conditions across LED, vehicle, and h-CTZ treatments in LMO7 and LMO11 expressing cultures.For each treatment, data were grouped into "pre" and "post" conditions.For each iteration of the test, we shuffled the data simulating the null hypothesis that presumes no difference between the conditions.After shuffling, the dataset was split again into "pre" and "post" groups, maintaining their original sizes, and the mean difference between these groups was calculated.This process was repeated 30,000 times to construct a null distribution of mean differences, representing the expected variability under the null hypothesis.The actual mean difference was calculated between the pre and post conditions for each treatment and group, comparing it with the null distribution.The p-value was calculated based on how the actual observed difference in means compared to the null distribution.Given the multiple comparisons involved across treatments and groups, we applied a Bonferroni correction to adjust the threshold for significance.

Coupling Efficiency of LMOs
To evaluate the performance of LMOs, whole-cell patch clamp recordings were obtained from cultured HEK293 cells expressing these constructs.For each recording, opsins were activated by an arc lamp to obtain the maximal photocurrent and by luciferin (CTZ, hCTZ, eCTZ) to obtain the bioluminescence-induced current [Fig.2(a)].We began by measuring, under voltage clamp conditions (−60 mV), the photocurrents evoked by exciting the opsin actuators directly via illumination by an arc lamp, choosing a filter cube matching the absorption peak of the opsin.As shown in the example in Fig. 2(b), for a cell expressing LMO7, illumination evoked an inward photocurrent due to activation of VChR1.This current reached a peak within a few ms and exhibited a sustained plateau that persisted for as long as the excitation light was maintained [1 s in the example shown in Fig. 2(b)].To determine the effectiveness of the LMO for chemogenetic control of membrane potential, we measured the ability of the luciferin to induce currents in these cells.Infusion of luciferin into the recording chamber yielded bioluminescence emission and simultaneous activation of an inward current [Fig.2(b)].This inward current generally tracked the time course of the luciferin presence in the chamber.We then used these measurements to determine the efficiency of coupling between the luciferase light source and the opsin actuator.We employed a simplified version of the procedure introduced by Berglund et al. 3 In brief, we compared the magnitude of currents induced by luciferin to those evoked by maximal exposure to light from an arc lamp by dividing the measured luciferin-induced current by the maximal photocurrent, yielding the coupling efficiency [Fig.2(c)].This value defines the intrinsic efficiency of coupling between luciferase and opsin and takes into account cell-to-cell variations in LMO expression.

Brightness of Light Emitter
In previous studies, we saw a continuous improvement of LMO function when replacing a luciferase with a brighter one.A 10-fold improvement in coupling efficiency was achieved when switching out wildtye GLuc (LMO2) with the brighter variant sbGLuc (LMO3), leading to the first excitatory LMO that allowed non-invasive manipulation of animal behavior. 5This trend continued, though not as dramatically, when we replaced sbGLuc in LMO3 with a luciferasefluorescent protein Förster resonance energy transfer (FRET) probe (NCS2, a fusion of eKL9h and mNeonGreen), resulting in LMO7. 21

Sensitivity of Light Sensor
We previously also saw an improvement of LMO function when replacing an opsin with a more light-sensitive one.Again, a 10-fold improvement in coupling efficiency was observed from LMO1 (Gluc-ChR2) to LMO2 (Gluc-VChR1). 3Thus, we expected to see an increase in coupling efficiency when we fused NCS2, the luciferase used successfully in LMO7 (NCS2-VChR1), channelrhodopsin ChRger3 23 in LMO8.The ChRger series of excitatory opsins was optimized  We next paired our currently brightest light emitter, GeNL_SS, with ChRmine, an opsin identified in a marine organism-based genomic screen for new classes of microbial opsins. 24hRmine was reported to have a hundred-fold improved operational light sensitivity compared with other fast, red-shifted variants.While combining GeNL_SS with VChR1 in LMO10 outperformed LMO7 (NCS2-VChR1), the combination with ChRmine in LMO11 (GeNL_SS-ChRmine) led to further improved coupling efficiency from 0.   three completely lacked a response to lamp stimulation, and two had a minimal response [Figs.6(c) and 6(d)].None of the cells showed any luciferin-induced current.This diminished response is reflected in the nonfunctional (n.f.) coupling efficiency of LMO7.3 (n ¼ 5).

Wavelength Compatibility
We previously generated a series of LMOs that utilize the red-shifted Renilla luciferase variant RLuc8.6-535(W156F)fused to an evolved red fluorescent protein (mCherry22.0,derived from mCherry with the mutations F11Y, Y38F, D59H, S62P, M66Q, L83F, K92T, V96E, W143T, E144T, T147S, I161T, Q163W, D174E, N196D, I197R, S203Y, and G219S; to be described fully in a manuscript currently in preparation), tethered to the C-terminus of various opsins, analogous to iLMO2. 4 mCherry22.0has peak excitation at 561 nm and peak emission at 593 nm with a quantum yield of ∼0.70, making it an excellent FRET acceptor for RLuc8.6-535.In LMO12, the peak emission of this red light emitter, 593 nm, closely matches the peak absorption of the opsin, ChRmine (585 nm 24 ).Even though LMO12 is constructed with a C-terminal fusion, we compared its performance to LMO11, which uses the light emitter GeNL_SS (peak emission around 520 nm) as an N-terminal fusion to ChRmine [Fig.7(a)] since these two LMO constructs contain the same opsin.While the photocurrent generated by light exposure from the arc lamp

LMO Performance in Activating Neuronal Populations
We used multi-electrode extracellular recordings to examine the ability of LMOs to activate neuronal populations.For these experiments, we transduced rat embryonic cortical neurons in MEA wells with AAV-hSyn-LMO, using a virus titer that yielded transduction of most plated neurons by LMOs. Figure 8 shows the effects of LED, vehicle, and CTZ treatments in spontaneously firing cultures on neuronal firing rates in LMO7 and LMO11 expressing cortical cultures.Different sets of neurons were assessed for each of the pre-and post-comparisons.Implementation of a permutation test, followed by a Bonferroni correction for multiple comparisons, provided a robust assessment of the significance of the observed changes between pre-and post-treatment conditions in the various groups.
Fig. 8 Multi-electrode recordings from cortical neurons transduced with AAV-hSyn-LMO7 and -LMO11.Average spiking frequencies of MEA channels before any treatment (pre) and after application (post) of physical or biological light, or vehicle.Spiking frequency increased when neurons were exposed to an LED light and with application of 10 μM CTZ but did not change with application of vehicle.
These results indicate that the optogenetic elements in LMOs 7 and 11 can be activated by both physical and biological light sources and that bioluminescence can provide sufficient excitatory drive to increase spontaneous activity in a population of neurons.

LMO Coupling Efficiency Versus Bioluminescence Light Emission
We previously found that radiance decreased for opsin-tethered light emitters, consistent with a loss of photon emission to direct energy transfer to the nearby opsin chromophore. 21We further observed a larger decrease for LMO7 (NCS2-VChR1) versus LMO3 (sbGLuc-VChR1).This is consistent with FRET from the light emitter to opsin being more efficient for NCS2 to VChR1 (LMO7) than for sbGLuc to VChR1 (LMO3).

Discussion
Here, we assessed the efficiencies in changing membrane potential of various LMOs consisting of different pairings of bioluminescent light emitters and light sensing opsins.Through whole cell patch clamp recordings in HEK293 cells, we determined the coupling efficiency for all tested LMOs, the amplitude of bioluminescence-driven inward current compared to the maximal photocurrent elicited by a physical light source (see Fig. 10 for summary).Through multielectrode array recordings in primary neurons, we confirmed that the findings in HEK293 cells broadly translated to application in neuronal populations.By comparing LMOs that differed in specific features, such as brightness of the light emitter, sensitivity of the light sensor, arrangement of moieties, and compatibility of emission/absorption spectra, we identified guiding principles of engineering LMOs that will be useful for future LMO designs.
Brightness of the light emitter was identified as critical early on in LMO designs. 5We and others are continuously working on generating ever brighter luminescent probes for multiple applications, including imaging with intact and split luciferases. 25,31We focused on engineering highly efficient FRET pairs between a luciferase donor and a fluorescent protein acceptor. 25Pairing of novel luciferase variants obtained through molecular evolution with mNeonGreen resulted in bright FRET-based light emission (sbALuc1-mNeonGreen, NCS1; 21 mNeonGreen-eKL9h, NCS2; 21 mNeonGreen-SSLuc, GeNL_SS25 25 ).Interestingly, when paired with VChR1 in an LMO, the coupling efficiency of NCS2 to VChR1 (LMO7) proved to be significantly higher than for NCS1 (LMO6), suggesting that the orientation of luciferase and fluorescent protein relative to the optogenetic channel may also be critical (i.e., mNeonGreen-eKL9h-VChR1 is superior to sbALuc1-mNeonGreen-VChR1). 21 We applied this principle successfully with LMOs 10 and 11 (mNeonGreen-SSLuc and GeNL_SS fused to VChR1 and ChRmine, respectively; this study).
We observed a "stepped" inward current for LMOs during bioluminescence-driven stimulation, especially for constructs incorporating GeNL_SS.We believe these steps reflect percent activation of total expressed LMO moieties in the patched cell.As luciferin perfuses into the recording chamber, more moieties are activated over time, increasing the observed inward current.We posit that stepped current traces are more prominent in GeNL_SS containing LMOs because the high light emission of the luciferase is enough to induce current change, even at low luciferin distribution.In contrast, weaker luciferases, such as sbGLuc, prompt all-or-none type responses, requiring a higher threshold of luciferin before inward current is observable.
It seems intuitively obvious that using a more light-sensitive opsin should increase coupling efficiency of LMOs.This has been borne out previously 3,20,22 and again in this study (LMO 10 versus LMO11).The only exception to this rule thus far is LMO8, which uses the designer opsin ChRger3. 23It is possible that the machine learning parameters chosen for an improved channelrhodopsin activated by a physical light source led to a reorientation of the retinal chromophore, making FRET-based activation by biological light sources less efficient.
In principle, the light emitter can be tethered to the N-or C-terminus of the opsin, and both options have led to robustly working LMOs.For instance, in our previous designs, the light emitter was always tethered to the N-terminus of the opsin, but for the inhibitory iLMO2 Tung et al. fused it to the C-terminus. 4 As the arrangement of moieties was never investigated in direct comparisons, we generated and tested LMO7 variants with N-(LMO7), C-(LMO7.2), or N-and C-(LMO7.3)terminal fusions of NCS2 to VChR1.Moving the light emitter to the C-terminus in LMO7.2 caused a considerable drop in coupling efficiency compared to the N-terminal fusion (LMO7).While access to the luciferin is likely a minor factor, as luciferins cross the cell membrane efficiently, the previous observation of differences due to orientation of luciferase and fluorescent protein relative to the channel may be critical here as well (LMO7: mNeonGreen-eKL9h-VChR1 versus LMO7.2:VChR1-mNeonGreen-eKL9h). Interestingly, attaching the light emitter to both termini seemed to interfere with the proper trafficking of the channel to the membrane (see representative fluorescent image of LMO7.3-expressingHEK cell [Fig.6(c)]) and possibly also with proper folding of the channel protein.A weak photocurrent was observed only sometimes, and bioluminescence-induced inward current could not be generated at all.In contrast, bioluminescence radiance from the two luciferases remained intact.
It appears obvious that this class of probes should benefit from higher compatibility of absorption and emission wavelengths of opsin and light emitter.However, most opsins have very wide absorbance spectra that extend activation far beyond their reported peak wavelengths, with high likelihood of activation across blue, green, and red wavelengths alike.VChR1, with an absorption peak of 535 nm, can be activated efficiently with sbGLuc (emission peak 480 nm), but activation is even more efficient with light emitters with emission peaks of 520 nm (NCS1, NCS2, GeNL_SS).Within the group of emitters with similar emission wavelength, we found significant differences in coupling efficiencies (NCS1 < NCS2 < GeNL_SS; Ref. 21 and this study) that cannot be explained simply by matching spectra between emitter and opsin.Another example is ChRmine that has an absorption peak at 585 nm.When paired with both a green (520 nm) and a red-shifted (589 nm) light emitter, ChRmine performs best in LMO11 with the green, brightest, N-terminally tethered light emitter (GeNL_SS) rather than with the dimmer, C-terminally tethered, but most well-matched emission wavelength emitter (mCh22.0-RLuc8.6) in LMO12.Some of these discrepancies may be due to differing folding efficiencies of the light emitters tested.
Overlapping emission and absorbance spectra of the donor and an acceptor in FRET is known to be of critical importance to maximize energy transfer efficiency.This has been studied mainly for FRET between small molecule fluorophores, between fluorescent proteins, or between a fluorescent and a bioluminescent protein.We hypothesize that FRET is the mechanism underlying the most efficient bioluminescent activation of opsins since this class of probes works reliably despite the fact that the absolute intensity of illumination by biological light sources is far lower than that which can be achieved using LEDs or lasers.If proximity of the two moieties is causing radiationless resonance energy transfer rather than simple, photon-mediated energy transfer, then the donor, the light emitter, will show loss of photon emission due to direct energy transfer to the opsin with efficient pairing, whereas it will recover emission when the acceptor, the opsin, is a less effective acceptor.This is supported by our observations that radiance of LMOs increases with decreasing coupling efficiency and vice versa [Ref.21 and this study (Fig. 9)].This is further supported by the experiments carried out by Berglund et al., where the luciferase moiety recovered bioluminescence after it was detached from the acceptor opsin through protease cleavage of the linker between luciferase and opsin. 22Future developments of improved LMOs might benefit from molecular evolution of fusion proteins to select for the most compatible FRET pairs of light emitters and opsins.
Ongoing advancements in identifying and evolving optogenetic actuators, 24,32 bioluminescent light emitters, 25 and luciferins enabling increased light emission and better penetration into the brain 33,34 offer a range of options for improving LMOs and broadening bioluminescent optogenetics applications.Our findings provide a basis for future engineering of highly efficient LMOs that tether bright fluorescent protein-luciferase constructs N-terminally to exceedingly light-sensitive opsins, selected for optimal FRET pairing through molecular evolution of the fusion proteins.We identified LMO11 (GeNL_SS-ChRmine) as a new and improved LMO for use in bioluminescent optogenetics-based projects.Finally, we demonstrate that whole cell patch clamp recording in HEK293 cells is an efficient strategy to quickly screen through LMO constructs.

Disclosures
The authors declare that they have no competing interests.

Fig. 1
Fig. 1 Luminopsin (LMO) features.(a) The luciferase-opsin fusion molecule (luminopsin) enables bimodal chemogenetic (CTZ) and optogenetic (LED) access to opsin activation.(b) Parameters for improving LMO performance are brightness of the light emitter, light sensitivity of the light sensor, and matching spectra for peak light emission and sensing.Moieties used in this study are indicated.(c) Possibilities for arrangement of moieties are N-terminal, C-terminal, or N-and C-terminal fusion of the luciferase to the opsin.

Fig. 2
Fig. 2 Quantifying LMO efficacy.(a) Membrane potential changes elicited chemo (CTZ)-or opto (LED, arc lamp)-genetically can be measured in HEK293 cells expressing an LMO.(b) In whole cell voltage patch clamp, inward current is determined in cells, here expressing LMO7, exposed to luciferin (hCTZ) and to light from an arc lamp (photocurrent).(c) Equation used to quantify LMO efficacy using currents measured in patch clamp.(d) Absence of effects of various luciferins and wavelengths of physical light source on the current of non-expressing HEK293 cells (controls, n ¼ 5).
photocurrent due to activation of VChR1.This current reached a peak within a few ms and exhibited a sustained plateau that persisted for as long as the excitation light was maintained [1 s in the example shown in Fig.2(b)].To determine the effectiveness of the LMO for chemogenetic control of membrane potential, we measured the ability of the luciferin to induce currents in these cells.Infusion of luciferin into the recording chamber yielded bioluminescence emission and simultaneous activation of an inward current [Fig.2(b)].This inward current generally tracked the time course of the luciferin presence in the chamber.We then used these measurements to determine the efficiency of coupling between the luciferase light source and the opsin actuator.We employed a simplified version of the procedure introduced by Berglund et al.3In brief, we compared the magnitude of currents induced by luciferin to those evoked by maximal exposure to light from an arc lamp by dividing the measured luciferin-induced current by the maximal photocurrent, yielding the coupling efficiency [Fig.2(c)].This value defines the intrinsic efficiency of coupling between luciferase and opsin and takes into account cell-to-cell variations in LMO expression.Figure 2(d) shows examples of non-expressing control HEK293 cells patched to determine the current response to light of different wavelengths and to different luciferins (CTZ, hCTZ, eCTZ).Examples are representative of five cells recorded for each experiment.
through a machine learning platform yielding high-photocurrent ChRs with high light sensitivity.While ChRger3 displayed a large response to lamp stimulation, it completely lacked a response to bioluminescence [n ¼ 5, Figs.4(c) and 4(d)].

Fig. 5
Fig. 5 Increasing both brightness of the light emitter and sensitivity of the light sensor.(a) Schematics of LMO10 and LMO11 with brightest luciferase-opsin fusion protein (GeNL_SS) and opsins VChR1 and the super light sensitive ChRmine.(b) Fluorescent images (left), photocurrent patch clamp traces (middle), and luciferin-induced patch clamp traces (right) for LMO10 and LMO11.(c) Coupling efficiencies of LMO10 and LMO11 (n ¼ 5).

Fig. 9
Fig.9Coupling efficiency versus bioluminescence produced by LMOs.Coupling efficiencies as determined throughout the above studies are plotted on the left, and bioluminescence measured from each LMO is plotted to the right.Bioluminescence produced by each LMO was measured in HEK293 cells in a plate reader with 100 μM concentration of luciferin (n ¼ 8 for each LMO).Readings were taken immediately after addition of substrate.Bioluminescence was normalized to expression of fluorescent reporter in each LMO using fluorescence ROI analysis in ImageJ.

Fig. 10
Fig. 10 Summary of patch clamp recordings in HEK293 cells.(a) Key features of LMOs tabulated in the order displayed in (b) and (c).(b) Representative example of luciferin-induced inward currents for each LMO tested.(c) Coupling efficiency graphs of LMOs tested.Red line in (b) and (c) indicates the level of performance of LMO3, the previously determined standard for a robustly functioning LMO.

Table 1
Summary of luminopsins assessed.

Table 2
Plasmids used in this paper.